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On the role of advection for the net exchange of CO2

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On the role of advection for the net exchange of CO

2

at a subalpine grassland in complex terrain

M. Galvagno, G. Wohlfahrt, E. Cremonese, U. Morra di Cella

Environmental Protection Agency of Aosta Valley - ARPA VdA Institute of Ecology - University of Innsbruck

EGU General Assembly, 10 April 2013

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• At mostFLUXNETsites, the net ecosystem CO2exchange is evaluated by means of eddy covariance (EC) using a set of instruments on a single tower.

• Assumptions: flat, horizontally homogeneous terrain and stationary conditions.

• Nighttime problem: low turbulent mixing, stable stratification, advective fluxes.

→Underestimation of nighttime net CO2exchange

Mass Balance Terms NEE=Fc+Fs+Fha+Fva

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• Eddy covariance measurements are challenging in non-ideal terrains, wheremountain ecosystemsare often naturally situated.

• No information exist on the role of advection at sites withshort canopies

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Study site

• Torgnon: Northwestern Italian Alps (Aosta Valley)

• Subalpine grassland (2160 m asl)

• EC measurements since 2008

• Maximum canopy height is 20 cm.

• Not located on a steep slope

• heterogeneous microtopography

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Study site

NE winds during nighttime SSW winds during daytime

DEM 20 cm resolution Isolines 2 m

∆ elevation ∼ 30 m

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Methods

Four control volumeswhere sequentially investigated during the growing season 2012:

1. Eddy covariance:

- 3D sonic anemometer (CSAT3) - Open-path IRGA (LI7500) placed at1.65 m agl - additional 2D anemometer placed at0.90 m agl

- 10 Hz data processed according to commonly accepted procedures

- Planar-fit method (Wilczak et al, 2001)

2. Profiling system and Chambers:

- Two vertical CO2profiles - Three measurement levels each (0.30, 0.80, 1.65 m agl)

- 30 meters uphill and downhill the EC tower along the different transects - Three ecosystem respiration automated chambers (LI8100, LICOR)

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Experimental scheme

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Data processing: mass balance terms

Eddy flux

Fca0 w0c0

Storage term

Fs=R1.65 0

∂c

∂tdz

Horizontal advection Fha=R1.65

0 u(z)∂c(z)∂x dz Vertical advection

Fva=wh1.65(ch1.65− [c])

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Results: Eddy fluxes

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Results: mass balance terms - mean diurnal variation

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Results: mass balance terms - nighttime values

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How to correct the nighttime problem?

It was not possible to identify an objective friction velocity threshold

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Alternative solutions

1 Using data when the maximum of Fc+Fsis observed in theeveningto develop relationships between NEE and independent variables, such as soil temperature (Van Gorsel et al 2007)

2 To add a constant advective offset to Fc+Fs

3 It appears that there are places, even in this kind of complex topography, where Fc+Fscaptures most ofthe actual nighttime respiration

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Conclusions

The main findings of this study are:

1 Fc+Fsconsiderably underestimates nighttime ecosystem respiration as measured by the automated ecosystem chambers.

2 Advection measurements indicate that horizontal, and to a lesser degree, vertical advection are important terms of the full mass balance during nighttime at the grassland site. During daytime advection appears to play a negligible role.

3 The NEE calculated by taking into account advection generally closely resembles nighttime ecosystem respiration as measured with chambers.

4 For two of the control volumes the order of magnitude of NEE computed with the mass balance approach (Fc+Fs+Fha+Fva) was not compatible with biotic fluxes measured by respiration chambers (as previously described for other sites e.g.

Aubinet et al 2010).

5 Ongoing work: testing the best correction approach

6 future 3D Experiments are planned to improve advection measurements.

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THANKS FOR YOUR ATTENTION

[email protected] www.arpa.vda.it www.biomet.co.at

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